Phonon dynamic behaviors induced by amorphous layers at heterointerfaces
An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials. While existing research has explored the impact of these layers on interfacial thermal transport, a comprehensive understanding of the underlying microscopic m...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2024-03, Vol.26 (1), p.8397-847 |
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creator | Wang, Quanjie Zhang, Jie Xiong, Yucheng Li, Shouhang Chernysh, Vladimir Liu, Xiangjun |
description | An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials. While existing research has explored the impact of these layers on interfacial thermal transport, a comprehensive understanding of the underlying microscopic mechanisms remains essential for advancing thermal nanodevice development. Through phonon wave packet simulations, we investigated the dynamic behaviors of phonons crossing the amorphous interlayer at the GaN/AlN interface from the mode level. Our results highlight the amorphous layer's capability to notably adjust the polarization properties of incoming phonons, culminating in phonon localization. By examining transmission outcomes on a per-mode basis, we demonstrate the amorphous layer's impediment on phonon transport. Notably, this resistance escalates with an increase in the amorphous layer thickness (
L
), with certain high-frequency TA phonons showing unexpectedly high transmissivity due to polarization conversion and inelastic scattering at the amorphous interface. In addition, we observe that the amorphous layer prompts multiple reflections of incident phonons, instigating discernible from the two-beam interference equation. Finally, in pursuit of enhanced phonon transport, we employ annealing techniques to optimize the interface morphology, leading to the recrystallization of the amorphous layer. This optimization yields a substantial enhancement of interfacial thermal conductance by up to 38% for
L
= 3 nm.
An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials. |
doi_str_mv | 10.1039/d3cp04480g |
format | Article |
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L
), with certain high-frequency TA phonons showing unexpectedly high transmissivity due to polarization conversion and inelastic scattering at the amorphous interface. In addition, we observe that the amorphous layer prompts multiple reflections of incident phonons, instigating discernible from the two-beam interference equation. Finally, in pursuit of enhanced phonon transport, we employ annealing techniques to optimize the interface morphology, leading to the recrystallization of the amorphous layer. This optimization yields a substantial enhancement of interfacial thermal conductance by up to 38% for
L
= 3 nm.
An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/d3cp04480g</identifier><identifier>PMID: 38407410</identifier><language>eng</language><publisher>England: Royal Society of Chemistry</publisher><subject>Dissimilar materials ; Heterostructures ; Inelastic scattering ; Interfaces ; Interlayers ; Nanotechnology devices ; Phonons ; Polarization ; Recrystallization ; Thermal conductivity ; Thermal mismatch ; Thickness ; Transmissivity ; Wave packets</subject><ispartof>Physical chemistry chemical physics : PCCP, 2024-03, Vol.26 (1), p.8397-847</ispartof><rights>Copyright Royal Society of Chemistry 2024</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c337t-c0cf90ba0df2e2638f8a432021f102128c7b5d8048ef5989189baaa018971f5b3</citedby><cites>FETCH-LOGICAL-c337t-c0cf90ba0df2e2638f8a432021f102128c7b5d8048ef5989189baaa018971f5b3</cites><orcidid>0000-0001-6023-785X ; 0000-0001-6287-8394</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/38407410$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Wang, Quanjie</creatorcontrib><creatorcontrib>Zhang, Jie</creatorcontrib><creatorcontrib>Xiong, Yucheng</creatorcontrib><creatorcontrib>Li, Shouhang</creatorcontrib><creatorcontrib>Chernysh, Vladimir</creatorcontrib><creatorcontrib>Liu, Xiangjun</creatorcontrib><title>Phonon dynamic behaviors induced by amorphous layers at heterointerfaces</title><title>Physical chemistry chemical physics : PCCP</title><addtitle>Phys Chem Chem Phys</addtitle><description>An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials. While existing research has explored the impact of these layers on interfacial thermal transport, a comprehensive understanding of the underlying microscopic mechanisms remains essential for advancing thermal nanodevice development. Through phonon wave packet simulations, we investigated the dynamic behaviors of phonons crossing the amorphous interlayer at the GaN/AlN interface from the mode level. Our results highlight the amorphous layer's capability to notably adjust the polarization properties of incoming phonons, culminating in phonon localization. By examining transmission outcomes on a per-mode basis, we demonstrate the amorphous layer's impediment on phonon transport. Notably, this resistance escalates with an increase in the amorphous layer thickness (
L
), with certain high-frequency TA phonons showing unexpectedly high transmissivity due to polarization conversion and inelastic scattering at the amorphous interface. In addition, we observe that the amorphous layer prompts multiple reflections of incident phonons, instigating discernible from the two-beam interference equation. Finally, in pursuit of enhanced phonon transport, we employ annealing techniques to optimize the interface morphology, leading to the recrystallization of the amorphous layer. This optimization yields a substantial enhancement of interfacial thermal conductance by up to 38% for
L
= 3 nm.
An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials.</description><subject>Dissimilar materials</subject><subject>Heterostructures</subject><subject>Inelastic scattering</subject><subject>Interfaces</subject><subject>Interlayers</subject><subject>Nanotechnology devices</subject><subject>Phonons</subject><subject>Polarization</subject><subject>Recrystallization</subject><subject>Thermal conductivity</subject><subject>Thermal mismatch</subject><subject>Thickness</subject><subject>Transmissivity</subject><subject>Wave packets</subject><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNpdkcFLwzAUxoMobk4v3pWCFxGqL03aJkeZOoWBO-i5pGliO9qmJq3Q_97MzQlevvfg_fj4-B5C5xhuMRB-VxDZAaUMPg7QFNOEhBwYPdzvaTJBJ86tAQDHmByjCWEUUophip5XpWlNGxRjK5pKBrkqxVdlrAuqthikKoJ8DERjbFeawQW1GJW_iT4oVa-sqVqvWkjlTtGRFrVTZ7s5Q-9Pj2_z53D5uniZ3y9DSUjahxKk5pALKHSkooQwzQQlEURYYy8Rk2keFwwoUzrmjGPGcyEE-JliHedkhq63vp01n4NyfdZUTqq6Fq3yCbOIb9yApsyjV__QtRls69NtqDRJeAzEUzdbSlrjnFU662zVCDtmGLJNv9kDma9--l14-HJnOeSNKvbob6EeuNgC1sn99e9B5BtP6n5V</recordid><startdate>20240306</startdate><enddate>20240306</enddate><creator>Wang, Quanjie</creator><creator>Zhang, Jie</creator><creator>Xiong, Yucheng</creator><creator>Li, Shouhang</creator><creator>Chernysh, Vladimir</creator><creator>Liu, Xiangjun</creator><general>Royal Society of Chemistry</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-6023-785X</orcidid><orcidid>https://orcid.org/0000-0001-6287-8394</orcidid></search><sort><creationdate>20240306</creationdate><title>Phonon dynamic behaviors induced by amorphous layers at heterointerfaces</title><author>Wang, Quanjie ; Zhang, Jie ; Xiong, Yucheng ; Li, Shouhang ; Chernysh, Vladimir ; Liu, Xiangjun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c337t-c0cf90ba0df2e2638f8a432021f102128c7b5d8048ef5989189baaa018971f5b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Dissimilar materials</topic><topic>Heterostructures</topic><topic>Inelastic scattering</topic><topic>Interfaces</topic><topic>Interlayers</topic><topic>Nanotechnology devices</topic><topic>Phonons</topic><topic>Polarization</topic><topic>Recrystallization</topic><topic>Thermal conductivity</topic><topic>Thermal mismatch</topic><topic>Thickness</topic><topic>Transmissivity</topic><topic>Wave packets</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, Quanjie</creatorcontrib><creatorcontrib>Zhang, Jie</creatorcontrib><creatorcontrib>Xiong, Yucheng</creatorcontrib><creatorcontrib>Li, Shouhang</creatorcontrib><creatorcontrib>Chernysh, Vladimir</creatorcontrib><creatorcontrib>Liu, Xiangjun</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, Quanjie</au><au>Zhang, Jie</au><au>Xiong, Yucheng</au><au>Li, Shouhang</au><au>Chernysh, Vladimir</au><au>Liu, Xiangjun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Phonon dynamic behaviors induced by amorphous layers at heterointerfaces</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><addtitle>Phys Chem Chem Phys</addtitle><date>2024-03-06</date><risdate>2024</risdate><volume>26</volume><issue>1</issue><spage>8397</spage><epage>847</epage><pages>8397-847</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials. While existing research has explored the impact of these layers on interfacial thermal transport, a comprehensive understanding of the underlying microscopic mechanisms remains essential for advancing thermal nanodevice development. Through phonon wave packet simulations, we investigated the dynamic behaviors of phonons crossing the amorphous interlayer at the GaN/AlN interface from the mode level. Our results highlight the amorphous layer's capability to notably adjust the polarization properties of incoming phonons, culminating in phonon localization. By examining transmission outcomes on a per-mode basis, we demonstrate the amorphous layer's impediment on phonon transport. Notably, this resistance escalates with an increase in the amorphous layer thickness (
L
), with certain high-frequency TA phonons showing unexpectedly high transmissivity due to polarization conversion and inelastic scattering at the amorphous interface. In addition, we observe that the amorphous layer prompts multiple reflections of incident phonons, instigating discernible from the two-beam interference equation. Finally, in pursuit of enhanced phonon transport, we employ annealing techniques to optimize the interface morphology, leading to the recrystallization of the amorphous layer. This optimization yields a substantial enhancement of interfacial thermal conductance by up to 38% for
L
= 3 nm.
An amorphous layer is commonly found at the interfaces of heterostructures due to lattice and thermal mismatch between dissimilar materials.</abstract><cop>England</cop><pub>Royal Society of Chemistry</pub><pmid>38407410</pmid><doi>10.1039/d3cp04480g</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0001-6023-785X</orcidid><orcidid>https://orcid.org/0000-0001-6287-8394</orcidid></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Dissimilar materials Heterostructures Inelastic scattering Interfaces Interlayers Nanotechnology devices Phonons Polarization Recrystallization Thermal conductivity Thermal mismatch Thickness Transmissivity Wave packets |
title | Phonon dynamic behaviors induced by amorphous layers at heterointerfaces |
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